Concepedia

Normal Stress Effects in Second-Order Fluids

Journal of Applied Physics · 1964 · 258 citations · 13 references

TL;DR

Second‑order fluids extend Newtonian fluid equations with viscoelastic corrections up to second order, characterized by three material constants (η₀, β, γ) besides density. The study demonstrates that the normal‑stress constant γ is governed by the shear‑relaxation modulus and proposes practical measurement techniques for β and γ. The authors propose several practical methods to determine the material constants β and γ. They find that γ is linked to the shear‑relaxation modulus and that in slow Couette flow the viscoelastic contribution to the normal thrust difference opposes the inertial contribution.

Abstract

In the general theory of the behavior of simple fluids with fading memory in slow deformations, the constitutive equation of those fluids called second-order fluids gives to the equation of Newtonian fluids a correction for viscoelastic effects that is complete to within terms of order greater than two in the time scale. The hydrodynamical behavior of incompressible second-order fluids is determined by three material constants: η0, β, γ, besides the density. We show here that not only the viscosity η0, but also the constant γ which governs certain normal stress effects, is determined by the shear-relaxation modulus of classical infinitesimal viscoelasticity. This result enables us to show that in a slow Couette flow the viscoelastic contribution to the difference in normal thrusts on the inner and outer cylindrical walls has a sign opposite to that of the inertial contribution. We also suggest several practicable methods for measuring β and γ.